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Key Factors for Dense Copper Coating by HVOF Spraying

Key Factors for Dense Copper Coating by HVOF Spraying

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place in preferential to the corrosion of copper coating (Eq.<br />

3) because the corrosion potential of these coatings were<br />

approximately –400 mV and close to that of the free steel<br />

plate at approximately –450 mV. On the other hand, the<br />

corrosion reaction of coating (Eq. 3) takes place exclusively<br />

and preferentially in case of not any and a slight amount of<br />

penetrating pores, respectively. This is because the corrosion<br />

reaction of steel substrate is negligible. This is the case <strong>for</strong> the<br />

copper coated steels under the Cond. C and D because their<br />

corrosion potentials corresponded to that of the free copper<br />

plate around –130 mV.<br />

These results revealed that the coating density at the<br />

fuel/oxygen ratio over 0.66 (Cond. C and D) improved more<br />

rapidly than that at the ratio below 0.56 (Cond. A and B). This<br />

fact implies that a certain important factor exists to improve<br />

the coating density, i.e. compactibility of sprayed particles at<br />

the fuel/oxygen ratio over 0.66. Such a factor was discussed in<br />

the next section.<br />

<strong>Factors</strong> to improve compactibility<br />

The compactness of <strong>HVOF</strong> spray coating was expected to<br />

depend mainly on the trans<strong>for</strong>mation degree of sprayed<br />

particles upon impinging, in other words, amounts of melted<br />

particles and highly de<strong>for</strong>mable particles.<br />

Typical results of capturing spray particles <strong>by</strong> agar gels are<br />

shown in Fig. 6. The spherical particles at the deeper positions<br />

corresponded to unmelted particles, which plunged into the<br />

agar gel without broken off. On the other hand, the fine<br />

particles at the shallower positions corresponded to melted<br />

particles, which were impinged to the gel target, broken into<br />

fine particles and solidified, resulted in being captured near the<br />

surface. As the fuel/oxygen ratio increases, the unmelted<br />

particles at the deeper positions decrease whereas the melted<br />

particles increase, as seen in Fig. 6. In order to show this<br />

phenomenon quantitatively, molten fractions of the sprayed<br />

particles were determined and represented in Fig. 7. At the<br />

ratio of 0.46 under the Cond. A, the molten fraction was 0 wt%.<br />

(<br />

Abundance ratio (%<br />

100<br />

80<br />

60<br />

40<br />

20<br />

TYPE2<br />

TYPE1<br />

TYPE4<br />

TYPE3<br />

0<br />

Cond. A B C D<br />

TYPE5<br />

Figure 10 Abundance ratios of five types splats under each<br />

condition.<br />

As the ratio increased, the molten fraction increased, especially<br />

considerably at the ratio of 0.87 (Cond. D). This rapid increase<br />

at the ratio of 0.87 (Cond.D) did not agree to the some<br />

experimental results that the compactibility of sprayed particles<br />

improved rapidly at the ratio of 0.66 (Cond. C), as mentioned<br />

above. Accordingly, the molten fraction was not a primary<br />

factor to improve the coating compactness under the <strong>HVOF</strong><br />

spray conditions in this paper although the molten fraction<br />

must play an important role on making a dense coating.<br />

The splat morphology is related to de<strong>for</strong>mability of sprayed<br />

particles. Figure 8 shows microscopic images of splats<br />

prepared under four spray conditions. The splats could be<br />

classified into some types of shapes such as lump, bullet<br />

wound and splash. As the fuel/oxygen ratio increased, the<br />

number of lump and bullet wound decreased whereas that of<br />

splash increased. In order to estimate the sprayed particle<br />

de<strong>for</strong>mability quantitatively, three-dimensional in<strong>for</strong>mation of<br />

the splats was collected <strong>by</strong> the laser microscopy. According to<br />

the height (or depth) and the area, the splats were classified<br />

into five types of shapes, as shown in Figure 9. In this figure,<br />

observed images are presented at the left side and their<br />

schemas are illustrated at the right side. The five types of splats<br />

are called as TYPE X <strong>for</strong> convenience below. The shape of<br />

TYPE 1 looks like bullet wound and is supposed to be <strong>for</strong>med<br />

<strong>by</strong> impinging of unmelted hard particles and <strong>by</strong> their falling<br />

apart. TYPE 2 is considered to be part of such hard particles<br />

sticking to the target. The shapes of both TYPE 3 and TYPE 4<br />

were caused <strong>by</strong> the unmelted particles soft enough to de<strong>for</strong>m<br />

plastically and their de<strong>for</strong>mation degrees may depend on<br />

temperature and impact <strong>for</strong>ce of the spray particle. The shape<br />

of TYPE5 is an extremely thin and flat and this is due to<br />

melting of particles. About 100 of splats were sampled<br />

randomly on the surface of test target sprayed under each<br />

condition. The numbers of splats were counted according to the<br />

above-mentioned classification and their abundance ratio was<br />

determined and shown in Fig. 10. The increase in abundance<br />

ratio of TYPE 5 is good agreement with the increase in molten<br />

fraction of melted particles at the ratio of fuel to oxygen of<br />

0.66 (Cond. D). This increase in the number of melted particles<br />

may be related to the result that the higher value was obtained<br />

especially under Cond. D on measuring the flight velocity of<br />

sprayed particles (see Fig. 1). When Cond. B is compared to<br />

Cond. C in terms of the abundance ratio, both TYPE 4 and<br />

TYPE 5 increases under Cond. C. However, the increasing rate<br />

<strong>for</strong> TYPE 4 is larger than that <strong>for</strong> TYPE 5. There<strong>for</strong>e, the<br />

reason why the compactibility of sprayed particles was<br />

improved rapidly under Cond. C is the increase of the<br />

unmelted particles soft enough to de<strong>for</strong>m plastically, in other<br />

words, with the sufficiently high plastic de<strong>for</strong>mability upon<br />

impinging.<br />

Conclusion<br />

In this study, we revealed that the key factors determining the<br />

compactness of sprayed particles in <strong>HVOF</strong> sprayed copper<br />

coatings. It is natural that the molten fraction of sprayed<br />

particles is important and the higher fraction leads to <strong>for</strong>m<br />

761

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